SUPPLEMENTARY GUIDANCE NOTE 4: WIND SHEAR

Size: px
Start display at page:

Download "SUPPLEMENTARY GUIDANCE NOTE 4: WIND SHEAR"

Transcription

1 A GOOD PRACTICE GUIDE TO THE APPLICATION OF ETSU-R-97 FOR THE ASSESSMENT AND RATING OF WIND TURBINE NOISE SUPPLEMENTARY GUIDANCE NOTE 4: WIND SHEAR ISSUE 1 JULY 2014 Page 1 of 14

2 PREFACE This document has been produced by a working group on behalf of the Institute of Acoustics consisting of the following members: Matthew Cand Robert Davis Chris Jordan Malcolm Hayes Richard Perkins Hoare Lea Acoustics RD Associates Northern Group Systems (Environmental Health) Hayes McKenzie Partnership Ltd. Parsons Brinckerhoff Ltd. The working group gratefully acknowledges the assistance provided by Gavin Irvine from Ion Acoustics Ltd in the drafting of this note. This supplementary guidance note has been produced to supplement the IOA document A GOOD PRACTICE GUIDE TO THE APPLICATION OF ETSU-R-97 FOR THE ASSESSMENT AND RATING OF WIND TURBINE NOISE which is available on the IOA website at the following link: (checked ). Prior to publication of this note, a peer review was undertaken by a separate group. Any comments on this document should be sent to ETSUCONSULT@IOA.ORG.UK. The IOA will keep the document under review, and consider updating when significant changes to current good practice have occurred. Richard Perkins Working Group Chairman & Editor. Institute of Acoustics 3rd Floor St Peter's House Victoria Street St. Albans Hertfordshire AL1 3WZ United Kingdom Supplementary Guidance Notes Number Title Information 1 Data Collection 2 Data Processing & Derivation of ETSU-R-97 background curves Equipment specifications; measurement surveys: Practical considerations and set-up guidance and examples. Data filtering, processing and regression analysis for different types of noise environments. 3 Sound Power Level Data Manufacturer s data and warranties analysis. 4 Wind Shear Wind speed references and long-term data analysis. 5 Post Completion measurements Examples, considerations and strategies. 6 Noise Propagation over water for on-shore wind turbines Noise propagation over large bodies of water. Page 2 of 14

3 CONTENTS Page 1 Context Background Scope of the Document Statutory Context 4 2 Wind Shear Wind Shear: Definitions Determining the Hub Height Wind Speed - general Method A: direct measurements Method B: calculations from other heights 5 3 Anemometry Data Checking Anemometry Data Time Stamps Check of Data Set Data from more than one anemometer or wind vane. 6 4 Deriving corrections for data referenced against wind data measured at 10 m m Measured Corrections Analysing long-term wind data Correcting the Turbine Noise Predictions Correcting background noise data 11 Page 3 of 14

4 1 Context 1.1 Background The Institute of Acoustics (IOA) published A GOOD PRACTICE GUIDE TO THE APPLICATION OF ETSU- R-97 FOR THE ASSESSMENT AND RATING OF WIND TURBINE NOISE (GPG) in May 2013 to provide technical assistance for the undertaking of wind turbine noise assessments using the ETSU-R-97 document. In order to keep the GPG to a reasonable length, but not to lose clarifications and case studies, it was decided to produce a number of supplementary guidance notes which would support the GPG This guidance note will be of relevance to: i. Acoustics consultants; ii. Local Planning Authority (LPA) Environmental Health and Planning departments; iii. Developers; iv. The Planning Inspectorate or equivalent regulating authority; v. The general public. 1.2 Scope of the Document A series of six Supplementary Guidance Notes have been produced. This Supplementary Guidance Note 4 supports Section 4.5 of the GPG. It provides additional information on the influence of wind shear on wind turbine noise assessments and provides guidance on analysing anemometry data and correcting for wind shear. The guidance note provides information on the following: 1.3 Statutory Context A short overview of the effect of wind shear on wind turbine noise assessments; Recommendations for analysing anemometry data; How to extrapolate the hub height wind speed from anemometry data at lower heights and; How data based on measured 10 m wind speed values can be corrected to account for wind shear This Supplementary Guidance Note has been approved by the IOA Council for use by IOA Members and others involved in the assessment and rating of wind turbine noise using ETSU-R-97. It covers technical matters of an acoustic nature which the IOA-NWG believes represent current good practice. 2 Wind Shear 2.1 Wind Shear: Definitions Wind shear is the variation in horizontal wind speed with height above ground level (agl). Under most conditions, wind speeds increase with height above ground and various equations can be used to describe this Turbine sound power levels determined in accordance with IEC are usually 1 reported with reference to standardised wind speeds at 10m height which are calculated from the hub height wind speeds using a standard equation (rather than actually measured at 10m height). This is therefore the key reference wind speed for wind turbine noise The GPG requires careful consideration of the wind speed used and how it was measured and derived. The requirement to determine wind speeds for background noise surveys is described in Section 2.6 of the GPG. This section sets out three methods, A, B or C (see GPG 2.6.3). Methods A or B are preferred. However, the use of a 10 m mast to measure wind speed (Method C) is still considered good practice for small-scale developments provided that wind shear is accounted for with appropriate corrections When wind speed values are determined at hub height (Method A or B) it is necessary to standardise them to 10 m height, for consistency of referencing with sound power data. That way, the turbine sound power levels (and therefore the predictions) and the background noise data (and associated noise limits) both refer to standardised wind speed which is derived from the hub height wind speed using Equation 1 below. 1 Please note that the 2012 edition 3 of IEC mainly requires sound power levels to be stated in relation to the hub height wind speed. Page 4 of 14

5 2.1.5 Standardising measured hub height (hh) wind speeds is done using the log-law equation with a standard roughness length, z 0 of 0.05m. This is Equation 1 below. As an example, if 6.7 m/s is measured at 80m height it would correspond to a standardised 10 m wind speed of 4.8 m/s. Equation 1 Where v 10 is the standardised 10 m height wind speed, v hh the hub height (hh) wind speed and z 0 the standard ground roughness length of 0.05m The ground roughness usually models the degree to which wind is slowed down by friction as it passes close to the ground: the rougher the ground (and the more obstacles such as trees, buildings etc.), the more the wind is slowed down and the larger the roughness length. For the standardisation process described in IEC and used therein, a fixed value of 0.05 is used in all cases for reference purposes Also relevant to wind farm noise assessments is the power law shown below Equation 2. Compared to Equation 1, this is an alternative mathematical representation used to model wind shear effects arising from differing atmospheric states. This model is now more frequently used when analysing long-term data as considered in the present SGN. Equation 2 Where v 1 is the wind speed at h 1 and v 2 is the wind speed at height h 2. The exponent m in the equation is known as the wind shear exponent. 2.2 Determining the Hub Height Wind Speed - general Methods A and B involve determining the hub height wind speed data from an anemometry mast or from a LiDAR or SoDAR unit, for every 10 min data point recorded during the noise survey. Once hub height is established (with Methods A or B), as stated above, it should be standardised to 10 m height (Equation 1). 2.3 Method A: direct measurements For method A, the hub height wind speed is obtained directly from measurements and no corrections are required, although the data should be checked for consistency and accuracy see section Method B: calculations from other heights Where there are no anemometers at or close to hub height, but measurements are available at two different heights (h1 and h2), hub height wind speeds can be estimated by extrapolation. The criteria for h 1 and h 2 for this to be applicable are set out in the GPG (2.6.3) To obtain the wind speed at hub height, Equation 2 can be re-arranged to determine the wind shear exponent m based on the known data (v 1, v 2, h 1, h 2 ) for each 10 minute data period. Equation 2, rearranged is shown below: log / log Equation The wind shear exponent m is then used in Equation 2 to estimate the wind speed at hub height from the upper height measured. Where the wind speed at the lower anemometer (v 1 at h 1 ) is higher than the higher anemometer (v 2 at h 2 ) then this calculation should not be performed and it is suggested that the hub height wind speed is set to the higher reading (i.e. assumption of zero rather than negative shear) Example of GPG method B: In this example, the mast has anemometers at 70 and 50 m height. In one particular 10 minute interval, average wind speeds of 6.4 and 5.7 m/s were measured respectively. Using Equation 3, this corresponds to a shear exponent of m=0.32. If the proposed turbine hub height is 80 m, then the wind speed at 80 m can be estimated from the measured 70 m wind speed (6.4 m/s) and m=0.32 using Equation 2. This results in a value of 6.7 m/s at 80 m height, or 4.8 m/s standardised The same formulae (Equations 2 and 3) can also be used to interpolate between two heights which are below and above the turbine hub height, such as for example with LiDAR/SODAR data. In all cases, the method used to determine the hub height wind speed should be clearly stated. Page 5 of 14

6 3 Anemometry Data 3.1 Checking Anemometry Data On receiving anemometry data, either for relating to measured background noise levels directly, or for longterm wind shear analysis, a number of checks need to be carried out to verify the data, as errors and missing data can occur. 3.2 Time Stamps Before carrying out the noise survey, a check should be made with the supplier/installer of the system regarding the operation of the anemometry system. In particular it will be necessary to establish that the time clock of the logger is accurately set and that anemometry system is functioning correctly and logging in 10-minute periods (see GPG 2.8) The loggers for anemometry masts are usually set up with the clock set to GMT all year (no daylight savings). However, this should be verified with those responsible for providing the data. It is also necessary to check whether the time stamps correspond to the start of the period or at end of a 10 minute period. This will vary from logger to logger On receiving the data, it is necessary to correct the data for the local time at the time of survey. The ETSU- R-97 amenity hours daytime periods and night-time relate to the local time at the time of the survey and therefore it is necessary to correct the time stamps of the data to the local time. Care should be taken to ensure that the periods when the clocks go forward or back are taken into account. 3.3 Check of Data Set The anemometry data must be checked for errors ideally, in the first instance, by specialists providing the data and then by the acoustic engineer. It is not unusual for data to include error values or for samples to be omitted from the data set. Sometimes, data is provided with missing periods or periods removed when error values occur and data with missing periods, if not corrected, will lead to synchronisation errors. Ideally, the time series provided for the wind data should be continuous with no missing periods. A new time sequence can be added adjacent to the data to check this. Data should be checked for error report values. Data from anemometry masts also can in some cases flat-line (constant readings) at low wind speed values. Careful inspection of the noise and wind speed time history plots can also provide a check that the data is synchronised and can help determine periods when error values occur LiDAR and SoDAR will also have error values due to low cloud or rain or other conditions and therefore the data must be first checked ideally by those providing the data. Section of the GPG describes the use of LiDAR and SoDAR data In addition, the anemometry mast data should be checked for errors or offsets in the wind direction. A mast installation report may specify any offsets that would need to be applied to the wind direction. Noting the wind direction whilst on site provides a check that the wind direction corresponds with that reported by the anemometry system. 3.4 Data from more than one anemometer or wind vane Anemometry masts will often have more than one wind sensor at some of the heights. In these cases, a choice must be made in carrying out any calculations, especially according to Method B Figure 1 below shows data from the ratio of wind speeds (v 1 /v 2 ) for two anemometers plotted against wind direction. Anemometer v 1 was at 62.5 meters mounted on the top of the mast whereas v 2 was located at 60 metres. It can be seen that for most wind directions, the difference between the two anemometers is small, but at around 90 there is a dip as the v 1 wind speeds are reduced due to the presence of a lightning conductor rod. At approximately 0, the mast tower shields anemometer v 2 and there is a larger disparity between the two readings When using such data for referencing background noise measurements, the resulting effects tend to be limited. But when undertaking wind shear analysis of long-term measurement data (see below), it is crucial to account for these shadowing effect or this can lead to unrealistic values which are spurious With large masts it is fairly common for several anemometers to be mounted on booms, e.g. with one orientated to the north and one orientated to the south. An analysis of the type shown in Figure 1 can allow the effects of the wind direction on the anemometer to be studied. In most cases, data from two anemometers at the same height can be averaged as reported in the GPG, but where shadowing effects Page 6 of 14

7 occur, data from the unshaded anemometer can be used for the wind directions where this occurs. If one anemometer is present instead of a pair, an analysis of average wind shear exponent as a function of wind direction can highlight a similarly narrow wind sector with atypical and unrealistic values of wind shear, and this data should be excluded from the analysis Although this is not generally necessary, it is noted that wind direction data from wind vanes should not be arithmetically averaged 2, and vector averaging should be used. It is sufficient to report only the results of the wind vane closest to the proposed hub height as recommended in the GPG (2.6). Figure 1 Blue: ratio of wind speeds measured by two anemometers installed at similar heights on an anemometry mast as a function of wind direction, showing spurious values for two narrow arcs (around 0 and 90 degrees from north). The yellow data samples correspond to low wind speeds (below 2.5 m/s) which have been removed to obtain a better correlation. 4 Deriving corrections for data referenced against wind data measured at 10 m m Measured Corrections As noted in the GPG (2.6.6), when a baseline noise survey has been referenced to measured 10 m data, it is necessary to apply corrections to account for wind shear effects As described in the GPG, the cost of erecting a tall anemometry mast (or similar) during the baseline survey may not be justified for the smaller wind turbine projects. In this case, the long-term data necessary to derive site-specific wind shear may not be available either. A simplified wind shear correction is described in paragraph of the IoA GPG. It involves shifting the turbine noise predictions to the left along the wind speed axis (i.e. at lower wind speeds than if direct predictions are used). This is an empirical method which should result in robust, that is conservative, noise assessments even in the absence of site-specific data. A tolerance of +5 m can be applied when considering the hub height thresholds in the GPG. The noise limits are then based on measured wind speeds at 10 m height However this method does not use actual site-specific wind shear conditions. In some cases, suitable site anemometry data may in fact be available: either from an anemometer on an adjacent (representative) site, or because historic data is available, or because a mast was erected after the noise assessment such that the original noise data can be re-analysed. In the case of using a nearby mast, it is suggested that this is within 5 km of the wind farm site, with careful consideration of factors such as topography and tree/ground obstacles cover, which have to be similar to the proposed site or significant differences can be observed. Note that use of longer-term data, typically at least one year duration, is considered good practice in this case. 2 Arithmetically averaging 355 and 5 will lead to an erroneous result of 180. Page 7 of 14

8 4.1.4 This section describes the associated methods of correcting for wind shear based on this data, which can be classified into two basic methods: Applying a correction to the turbine noise predictions this involves shifting the turbine noise predictions to the left along the wind speed axis (decreased wind speeds for a given prediction). This method is similar to that described in the GPG Paragraph but using derived site-specific wind shear values rather than a simple fixed correction. Alternatively, the background noise data can be corrected based on measured wind shear values this involves shifting the background noise data to the right along the wind speed axis (increased wind speeds for a given background level) Note that the former is used more often (see 4.4). Applying a correction to the noise predictions means that background noise values are still referenced to the measured wind speed at 10 m height. Alternatively, shifting the background noise data effectively results in noise limits set in relation to a specific hub height (for which the wind speed is standardised to 10 m). In each case, it is important that the noise conditions limits clearly set out the appropriate wind speed reference and that consistency of wind references is retained (see of the GPG). Those responsible for preparing the noise assessment will have to justify firstly why a 10 m mast was used and secondly the wind shear correction method used At the end of this Supplementary Guidance Note, example wind shear exponents (Equation 3) are set out based on the analysis of long-term wind data from anemometry masts from various sites. This data is provided for reference only, so that the results of wind shear calculations can be compared with typical examples from other sites. It may be tempting to use such data to provide corrections required in some cases; however, this approach is not recommended because wind shear data is variable from site to site and the use of generic wind shear data would lead to arguments and inconsistencies. Therefore, unless a source of wind speed data is available for the actual turbine site or a similar site to it, the simplified approach advocated in the GPG Section should be used. 4.2 Analysing long-term wind data With a source of wind data, an analysis of the wind shear corrections can be determined. Typically datasets of 1 year or more are used, and it is recommended that at least six months of wind data 3, comprising both winter and summer months, is obtained. The use of database software is particularly suitable for the analysis of such large datasets. The requirements for the anemometry source (measurement heights etc.) should be as set out in the GPG (2.6.3) Firstly, both the hub height wind speed and actual 10 m wind speed need to be calculated for each 10 minute period. The hub height wind speed can be determined in the way set out in the GPG (2.6.4), and then standardised using Equation Some masts will have an anemometer at 10 m height and therefore this information can be used directly. If there is no 10 m anemometer, the 10 m wind speed should be calculated by extrapolation from the nearest (i.e. lowest) anemometer using the power law (Equation 2 and 3), in a similar way to that set out in section 2.4 above (Method B, but h1 and h2 being the two lowest anemometers). The same applies if hub height is not directly measured by the mast When performing this kind of analysis, the data must be filtered to remove erroneous or unrepresentative data as described in Section 3. See in particular the comments above on mast shadowing which can lead to erroneous shear coefficients. Data with negative wind shear, i.e. where the wind speed at the higher height is not greater than measured at the lower height, can also be excluded from the averaging or alternatively, a value of zero wind shear is assumed (constant wind speed with height). This provides a more conservative analysis The wind shear is then calculated either through: The exponent (m) between the hub height and 10 m wind speeds, using the average wind speed for the 10 minute periods considered (see 4.2.8) and Equation 3. 3 Ray, M. L., A. L. Rogers, and J. G. McGowan. "Analysis of wind shear models and trends in different terrains." University of Massachusetts, Department of Mechanical and Industrial Engineering, Renewable Energy Research Laboratory (2006). Page 8 of 14

9 The difference (subtraction) between the actual/extrapolated 10 m wind speed and that obtained from standardising the hub height wind speed (using Equation 1) for each of the 10 minute periods considered Example1 : In this example, the mast has anemometers at hub height (64 m) and 10 m height directly. In one particular 10 minute interval, wind speeds of 5.1 and 3.0 m/s are measured respectively. This corresponds to a wind shear exponent of 0.29 (Equation 3) between 64 m and 10 m. Alternatively, the difference between the measured 10 m wind speed and the standardised 64 m height wind speed (3.8 m/s) is calculated as 0.8 m/s. Example 2: Same as above but there are no measurements at 10 m height. However the mast has anemometers at 30 and 20 m height in addition to 64 m height. From the measurements at 30 and 20 m (4 and 3.4 m/s respectively), an exponent of 0.4 is determined and used to calculate a wind speed of 2.6 m/s at 10 m by extrapolation (Equation 2) from the 20 m measurements. This represents an exponent of 0.37 (between 64 and 10 m/s) or a shift of -1.2 m/s with the standardised wind speed of 3.8 m/s It can be seen from the illustrative examples at the end of this SGN that wind shear can be strongly dependant on wind speed, as increased winds tend in particular to disturb stable atmospheric conditions. High shear exponents may be apparent in conditions in which no turbines would operate. Averaging data for all wind speeds may therefore result in unrealistic values. The data should therefore be binned into 1 m/s wide bins for each integer wind speed value. If the purpose of the data analysis is to find appropriate corrections to measured 10 m wind speeds, the data should be binned according to this reference. If the intent is to correct emission or predictions values (which are based on standardised wind speeds), the binning should be made according to standardised wind speeds The wind shear data (exponents or direct wind speed difference values) are then averaged for different key periods: ETSU-R-97 evening periods (18.00 to 23.00) and ETSU-R-97 night-time periods ( ). During these periods, wind shear due to atmospheric effects tends to be highest and seasonal effects are more limited. The standard deviation of the variations around the average should also be determined to evaluate variability; it is typically of the order of 50% of the average values. 4.3 Correcting the Turbine Noise Predictions This method involves shifting the turbine noise predictions to the left along the wind speed axis. The calculated wind shear correction values are applied to the wind speed reference used for predictions of wind turbine noise. This can be done either by adjusting the source levels (emissions) or the predictions at each location (immissions). An interpolation is then required to obtain values at integer wind speeds An example calculation of corrections applied to manufacturer sound power data is shown in Figure 2. The correction is shown for average wind shear values, determined as a function of standardised wind speed bins, and the same process can be undertaken for the average +/- one standard deviation.it can be seen from this example that, for a variable speed turbine, the effects of wind shear only significantly affect the effective emission levels at lower wind speeds, below the maximum noise output of the turbine. The sound power data for integer wind speeds can then be determined for example by linear interpolation (as shown in Figure 2). In addition to the average shear correction, consideration of plus and minus one standard deviation provides a reasonable account of what may occur during less frequent periods. The assessment will then be based on the values with the highest shift, i.e. including the standard deviation. For example: from the standardised wind speed of 4 m/s, the corresponding hub height (80 m) wind speed is determined (5.6 m/s) using Equation 1. At this standardised wind speed, an exponent of 0.3 was determined as representative of the average shear at the site. This is used to calculate a wind speed of 3.1 m/s at 10 m height from the hub height wind speed using Equation 2, or a shift of = 0.9 m/s. If a variation of one standard deviation around the average shear is considered (approximately 50 % more in this example), this corresponds to a worst-case shift of 1.3 m/s to 2.7 m/s. The sound power at the standardised wind speed (99 db(a)) is expressed at the shifted wind speed of 2.7 m/s It is equally valid to correct the turbine noise predictions instead of adjusting the source levels. In the example below in Figure 3, turbine noise predictions are shifted for an average wind shear value. As above, this can be calculated from the derived exponent values, or directly from the calculated differences between actual and standardised 10 m wind speeds, and using corrections for average shear plus one standard deviation. Page 9 of 14

10 Standardised wind speed Hub Height (m) 80 Sound power Corresponding hub height wind speed Site Shear Exponent (average) m height wind speed, using average shear m height wind speed, using average+stdev shear Interpolated at integer 10 m wind speed Sound power, db(a) Sound Power Corrected for average and stdev shear Corrected for average shear Interpolated Wind speed at 10 m height (standardised or measured, m/s) Table 1 & Figure 2 turbine sound power adjusted for derived wind shear values at different wind speeds values at integer wind speeds are then determined by linear interpolation (green squares) Noise Level L 90 db(a) y = E-04x E-02x E-01x E+00x E Wind Speed at 10 m (m/s) Figure 3 Chart of background noise levels against measured 10 m wind speeds (open grey circles), the best fit curve (thin black line) to this data, the derived noise limit curve (thick black line) during amenity hours day time periods. Predicted immission noise levels (thick dashed lines with open circles): standard shear conditions (green) and corrected for specific average shear (blue, error bars represent 1 standard deviation from the average). Page 10 of 14

11 4.4 Correcting background noise data Although the above correction to predictions (section 4.3) is used more often, noise data measured in relation to 10 m height wind speed during the survey can be adjusted to hub height (standardised), to account for wind shear. Using this method, the background noise is corrected based on measured wind shear exponents obtained from the analysis of long-term anemometry data obtained as set out above. In this case, the derived background noise curve is adjusted to a specific hub height wind speed and therefore the noise limits derived from this data, using the ETSU-R-97 method, will be set relative to a specific hub height, which is then standardised for referencing. The method is as follows: As noted above in 4.2.7, in this case the analysis of long-term shear data is made by binning data according to measured (or extrapolated) 10 m wind speed (rather than standardised wind speeds). For each 10-minute value, determine the hub-height wind speed from the measured wind speed at 10 m height using either the derived shift or wind shear exponent (m) (Equation 2), for the corresponding wind speed bin and time of day. For consistency with the method of 4.3 and to obtain a conservative result, it is recommended that the wind shear used for the correction is the average value plus one standard deviation for each of the wind speed bins. The hub height wind speed is then standardised to 10 m height for referencing. A trend-line to this adjusted data can then be produced in the usual way. If the full dataset is not available, the derived trendline is corrected directly. Page 11 of 14

12 Illustrative Examples of Wind Shear Analysis (Figures 4 & 5) ** NB: Examples shown for qualitative and illustrative purposes ** Page 12 of 14

13 The example data below is shown for comparative reference but should not be used directly for corrections in the absence of site-specific data. The values shown are averaged wind shear exponents (Equation 3) obtained following analysis of long-term measured mast data. The standard deviation around the average is typically around 50% of the average at lower wind speeds. Central England Location; Yearly Average; Moderate tree cover in relatively flat location Buildings located within 600m. High Ridgeline/Tall Hill Location; Yearly Average; Clear Hill Top. UK East Coast Flat Landscape; Yearly Average; Limited Tree cover. Coastal Location; Yearly Average; End of Long Harbour Wall: >1km from Coast. Coastal Plain; Yearly Average; Western Side UK: No trees or buildings. Standardised wind speed Wind Speed at 10 m All Data Amenity Night All Data Amenity Night All Data Amenity Night All Data Amenity Night All Data Amenity Night East Anglia; All Data Yearly Average; Amenity Rural tree lined boundaries. Night Table 2: Typical averaged wind shear exponents Page 13 of 14

14 Page 14 of 14 SUPPLEMENTARY GUIDANCE NOTE 4: WIND SHEAR

Wind shear and its effect on wind turbine noise assessment Report by David McLaughlin MIOA, of SgurrEnergy

Wind shear and its effect on wind turbine noise assessment Report by David McLaughlin MIOA, of SgurrEnergy Wind shear and its effect on wind turbine noise assessment Report by David McLaughlin MIOA, of SgurrEnergy Motivation Wind shear is widely misunderstood in the context of noise assessments. Bowdler et

More information

MICROPHONE WIND SPEED LIMITS DURING WIND FARM NOISE MEASUREMENTS

MICROPHONE WIND SPEED LIMITS DURING WIND FARM NOISE MEASUREMENTS MICROPHONE WIND SPEED LIMITS DURING WIND FARM NOISE MEASUREMENTS Abstract Jon Cooper 1 and Tom Evans 2 1 Resonate Acoustics, Level 1/23 Peel St, Adelaide SA 5000, Australia Email: jon.cooper@resonateacoustics.com

More information

7 th International Conference on Wind Turbine Noise Rotterdam 2 nd to 5 th May 2017

7 th International Conference on Wind Turbine Noise Rotterdam 2 nd to 5 th May 2017 7 th International Conference on Wind Turbine Noise Rotterdam 2 nd to 5 th May 2017 Sound power level measurements 3.0 ir. L.M. Eilders, Peutz bv: l.eilders@peutz.nl ing. E.H.A. de Beer, Peutz bv: e.debeer@peutz.nl

More information

Dick Bowdler Acoustic Consultant

Dick Bowdler Acoustic Consultant Dick Bowdler Acoustic Consultant 01383 882 644 077 8535 2534 dick@dickbowdler.co.uk WIND SHEAR AND ITS EFFECT ON NOISE ASSESSMENT OF WIND TURBINES June 2009 The Haven, Low Causeway, Culross, Fife. KY12

More information

Influence of wind direction on noise emission and propagation from wind turbines

Influence of wind direction on noise emission and propagation from wind turbines Influence of wind direction on noise emission and propagation from wind turbines Tom Evans and Jonathan Cooper Resonate Acoustics, 97 Carrington Street, Adelaide, South Australia 5000 ABSTRACT Noise predictions

More information

EWEA Noise Wind Turbine Noise Workshop

EWEA Noise Wind Turbine Noise Workshop EWEA Noise Wind Turbine Noise Workshop Pre- and Post Construction Noise Measurements Dr Andy McKenzie Hayes McKenzie Partnership Ltd Salisbury & Machynlleth UK Wind Turbine Noise Planning ETSU-R-97 X db

More information

Wind Turbine Noise Measurements How are Results influenced by different Methods of deriving Wind Speeds? Sylvia Broneske

Wind Turbine Noise Measurements How are Results influenced by different Methods of deriving Wind Speeds? Sylvia Broneske INTERNOISE 2014 16 19 November in Melbourne, Australia Wind Turbine Noise Measurements How are Results influenced by different Methods of deriving Wind Speeds? Sylvia Broneske Hayes McKenzie Partnership

More information

Influence of non-standard atmospheric conditions on turbine noise levels near wind farms

Influence of non-standard atmospheric conditions on turbine noise levels near wind farms Influence of non-standard atmospheric conditions on turbine noise levels near wind farms Jonathan COOPER 1 ; Tom EVANS 1 ; Vahid ALAMSHAH 1 1 Resonate Acoustics, Australia ABSTRACT This paper investigates

More information

A review of Australian wind farm noise assessment procedures

A review of Australian wind farm noise assessment procedures Proceedings of ACOUSTICS 2016 9-11 November 2016, Brisbane, Australia A review of Australian wind farm noise assessment procedures Tom Evans 1 and Jon Cooper 2 1 Resonate Acoustics, Level 4, 10 Yarra Street,

More information

Validation of Measurements from a ZephIR Lidar

Validation of Measurements from a ZephIR Lidar Validation of Measurements from a ZephIR Lidar Peter Argyle, Simon Watson CREST, Loughborough University, Loughborough, United Kingdom p.argyle@lboro.ac.uk INTRODUCTION Wind farm construction projects

More information

The effect of a common wind shear adjustment methodology on the assessment of wind farms when applying ETSU-R-97

The effect of a common wind shear adjustment methodology on the assessment of wind farms when applying ETSU-R-97 The effect of a common wind shear adjustment methodology on the assessment of wind farms when applying ETSU-R-97 by Mike Stigwood, MAS Environmental (MAS) 27 th September 2011 Executive summary This research

More information

CORRELATION EFFECTS IN THE FIELD CLASSIFICATION OF GROUND BASED REMOTE WIND SENSORS

CORRELATION EFFECTS IN THE FIELD CLASSIFICATION OF GROUND BASED REMOTE WIND SENSORS CORRELATION EFFECTS IN THE FIELD CLASSIFICATION OF GROUND BASED REMOTE WIND SENSORS Will Barker (1), Julia Gottschall (2), Michael Harris (3), John Medley (4), Edward Burin des Roziers (5), Chris Slinger

More information

3D Nacelle Mounted Lidar in Complex Terrain

3D Nacelle Mounted Lidar in Complex Terrain ENERGY 3D Nacelle Mounted Lidar in Complex Terrain PCWG Hamburg, Germany Paul Lawson 25.03.2015 1 DNV GL 125.03.2015 SAFER, SMARTER, GREENER Agenda Introduction and Project Background Lidar Specifications

More information

Wind Project Siting & Resource Assessment

Wind Project Siting & Resource Assessment Wind Project Siting & Resource Assessment David DeLuca, Project Manager AWS Truewind, LLC 463 New Karner Road Albany, NY 12205 ddeluca@awstruewind.com www.awstruewind.com AWS Truewind - Overview Industry

More information

Windcube FCR measurements

Windcube FCR measurements Windcube FCR measurements Principles, performance and recommendations for use of the Flow Complexity Recognition (FCR) algorithm for the Windcube ground-based Lidar Summary: As with any remote sensor,

More information

PROJECT CYCLOPS: THE WAY FORWARD IN POWER CURVE MEASUREMENTS?

PROJECT CYCLOPS: THE WAY FORWARD IN POWER CURVE MEASUREMENTS? Title Authors: Organisation PROJECT CYCLOPS: THE WAY FORWARD IN POWER CURVE MEASUREMENTS? Simon Feeney(1), Alan Derrick(1), Alastair Oram(1), Iain Campbell(1), Gail Hutton(1), Greg Powles(1), Chris Slinger(2),

More information

Executive Summary of Accuracy for WINDCUBE 200S

Executive Summary of Accuracy for WINDCUBE 200S Executive Summary of Accuracy for WINDCUBE 200S The potential of offshore wind energy has gained significant interest due to consistent and strong winds, resulting in very high capacity factors compared

More information

Available online at ScienceDirect. Energy Procedia 53 (2014 )

Available online at   ScienceDirect. Energy Procedia 53 (2014 ) Available online at www.sciencedirect.com ScienceDirect Energy Procedia 53 (2014 ) 156 161 EERA DeepWind 2014, 11th Deep Sea Offshore Wind R&D Conference Results and conclusions of a floating-lidar offshore

More information

The Wind Resource: Prospecting for Good Sites

The Wind Resource: Prospecting for Good Sites The Wind Resource: Prospecting for Good Sites Bruce Bailey, President AWS Truewind, LLC 255 Fuller Road Albany, NY 12203 bbailey@awstruewind.com Talk Topics Causes of Wind Resource Impacts on Project Viability

More information

Site Summary. Wind Resource Summary. Wind Resource Assessment For King Cove Date Last Modified: 8/6/2013 By: Rich Stromberg & Holly Ganser

Site Summary. Wind Resource Summary. Wind Resource Assessment For King Cove Date Last Modified: 8/6/2013 By: Rich Stromberg & Holly Ganser Site Summary Wind Resource Assessment For King Cove Date Last Modified: 8/6/2013 By: Rich Stromberg & Holly Ganser Station ID: 2857 Latitude: 55 7 45.8 N Longitude: 162 16 10.6 W Tower Type: 30 m NRG Tall

More information

Full Classification acc. to IEC for SoDAR AQ510 Wind Finder. Vincent Camier, Managing Director, Ammonit Measurement GmbH

Full Classification acc. to IEC for SoDAR AQ510 Wind Finder. Vincent Camier, Managing Director, Ammonit Measurement GmbH Full Classification acc. to IEC 61400-12-1 for SoDAR AQ510 Wind Finder Vincent Camier, Managing Director, Ammonit Measurement GmbH Ammonit Company Profile German company, based in Berlin +25 years of know-how

More information

LiDAR Application to resource assessment and turbine control

LiDAR Application to resource assessment and turbine control ENERGY LiDAR Application to resource assessment and turbine control Dr. Avishek Kumar The New Zealand Wind Energy Conference 13 th April 2016 1 SAFER, SMARTER, GREENER Agenda What is LiDAR? Remote Sensing

More information

Wind Resource Assessment for FALSE PASS, ALASKA Site # 2399 Date last modified: 7/20/2005 Prepared by: Mia Devine

Wind Resource Assessment for FALSE PASS, ALASKA Site # 2399 Date last modified: 7/20/2005 Prepared by: Mia Devine 813 W. Northern Lights Blvd. Anchorage, AK 99503 Phone: 907-269-3000 Fax: 907-269-3044 www.aidea.org/wind.htm Wind Resource Assessment for FALSE PASS, ALASKA Site # 2399 Date last modified: 7/20/2005 Prepared

More information

Computational Fluid Dynamics

Computational Fluid Dynamics Computational Fluid Dynamics A better understanding of wind conditions across the whole turbine rotor INTRODUCTION If you are involved in onshore wind you have probably come across the term CFD before

More information

Increased Project Bankability : Thailand's First Ground-Based LiDAR Wind Measurement Campaign

Increased Project Bankability : Thailand's First Ground-Based LiDAR Wind Measurement Campaign Increased Project Bankability : Thailand's First Ground-Based LiDAR Wind Measurement Campaign Authors: Velmurugan. k, Durga Bhavani, Ram kumar. B, Karim Fahssis As wind turbines size continue to grow with

More information

Wake effects at Horns Rev and their influence on energy production. Kraftværksvej 53 Frederiksborgvej 399. Ph.: Ph.

Wake effects at Horns Rev and their influence on energy production. Kraftværksvej 53 Frederiksborgvej 399. Ph.: Ph. Wake effects at Horns Rev and their influence on energy production Martin Méchali (1)(*), Rebecca Barthelmie (2), Sten Frandsen (2), Leo Jensen (1), Pierre-Elouan Réthoré (2) (1) Elsam Engineering (EE)

More information

Meteorological Measurements OWEZ

Meteorological Measurements OWEZ Meteorological Measurements OWEZ Half year report 01-01-2008-30-06-2008 H. Korterink P.J. Eecen ECN-E--08-062 OWEZ_R_121_20080101-20080630_wind_resource_2008_1 Abstract NoordzeeWind carries out an extensive

More information

3D Turbulence at the Offshore Wind Farm Egmond aan Zee J.W. Wagenaar P.J. Eecen

3D Turbulence at the Offshore Wind Farm Egmond aan Zee J.W. Wagenaar P.J. Eecen 3D Turbulence at the Offshore Wind Farm Egmond aan Zee J.W. Wagenaar P.J. Eecen OWEZ_R_121_3Dturbulence_20101008 ECN-E--10-075 OCTOBER 2010 Abstract NoordzeeWind carries out an extensive measurement and

More information

Meteorological Measurements OWEZ

Meteorological Measurements OWEZ Meteorological Measurements OWEZ Half year report - 01-07-2008-31-12-2008 H. Korterink P.J. Eecen J.W. Wagenaar ECN-E--09-018 OWEZ_R_121_20080701-20081231_WIND_RESOURCE_2008_2 Abstract NoordzeeWind carries

More information

Testing and Validation of the Triton Sodar

Testing and Validation of the Triton Sodar Testing and Validation of the Triton Sodar September 24, 2008 AWEA Resource Assessment Workshop Ron Nierenberg, Consulting Meteorologist Liz Walls, Second Wind Inc. Ron Consulting Nierenberg Meteorologist

More information

Measuring power performance with a Wind Iris 4- beam in accordance with EUDP procedure

Measuring power performance with a Wind Iris 4- beam in accordance with EUDP procedure Measuring power performance with a Wind Iris 4- beam in accordance with EUDP procedure This document evaluates the applicability of the EUDP procedure for wind turbine measuring power performance using

More information

VISUAL AIDS FOR DENOTING OBSTACLES

VISUAL AIDS FOR DENOTING OBSTACLES CHAPTER 6. VISUAL AIDS FOR DENOTING OBSTACLES 6.1 Objects to be marked and/or lighted Note. The marking and/or lighting of obstacles is intended to reduce hazards to aircraft by indicating the presence

More information

WIND DATA REPORT. Bourne Water District

WIND DATA REPORT. Bourne Water District WIND DATA REPORT Bourne Water District July to September 2010 Prepared for Massachusetts Clean Energy Center 55 Summer Street, 9th Floor Boston, MA 02110 by Dylan Chase James F. Manwell Utama Abdulwahid

More information

M. Mikkonen.

M. Mikkonen. Wind study by using mobile sodar technology M. Mikkonen Oulu University of Applied Sciences, School of Engineering, Oulu, Finland t3mimi00@students.oamk.com Abstract In this paper is presented a concept

More information

Supplement of Wind turbine power production and annual energy production depend on atmospheric stability and turbulence

Supplement of Wind turbine power production and annual energy production depend on atmospheric stability and turbulence Supplement of Wind Energ. Sci., 1, 221 236, 2016 http://www.wind-energ-sci.net/1/221/2016/ doi:10.5194/wes-1-221-2016-supplement Author(s) 2016. CC Attribution 3.0 License. Supplement of Wind turbine power

More information

Remote sensing standards: their current status and significance for offshore projects

Remote sensing standards: their current status and significance for offshore projects Remote sensing standards: their current status and significance for offshore projects Peter J M Clive Technical Development Consultant SgurrEnergy Ltd 225 Bath Street Glasgow G2 4GZ E: peter.clive@sgurrenergy.com

More information

Status: Rev: Comments Date: Author: Reviewer:

Status: Rev: Comments Date: Author: Reviewer: MT EMERALD WIND FARM REVISED A-WEIGHTED NOISE ASSESSMENT Rp 002 R01 2015545ML 30 January 2017 6 Gipps Street Collingwood VIC 3066 Australia T: +613 9416 1855 ABN: 53 470 077 191 www.marshallday.com Project:

More information

Outline. Wind Turbine Siting. Roughness. Wind Farm Design 4/7/2015

Outline. Wind Turbine Siting. Roughness. Wind Farm Design 4/7/2015 Wind Turbine Siting Andrew Kusiak 2139 Seamans Center Iowa City, Iowa 52242-1527 andrew-kusiak@uiowa.edu Tel: 319-335-5934 Fax: 319-335-5669 http://www.icaen.uiowa.edu/~ankusiak Terrain roughness Escarpments

More information

Buckland Wind Resource Report

Buckland Wind Resource Report Buckland Wind Resource Report By: Douglas Vaught, P.E., V3 Energy LLC, Eagle River, Alaska Date: September 17, 2010 Buckland met tower; D. Vaught photo Contents Summary... 2 Test Site Location... 2 Photographs...

More information

WIND DATA REPORT. Vinalhaven

WIND DATA REPORT. Vinalhaven WIND DATA REPORT Vinalhaven January - December, 2003 Prepared for Fox Islands Electric Cooperative by Anthony L. Rogers May 12, 2004 Report template version 1.1 Renewable Energy Research Laboratory 160

More information

Wind Farm Blockage: Searching for Suitable Validation Data

Wind Farm Blockage: Searching for Suitable Validation Data ENERGY Wind Farm Blockage: Searching for Suitable Validation Data James Bleeg, Mark Purcell, Renzo Ruisi, and Elizabeth Traiger 09 April 2018 1 DNV GL 2014 09 April 2018 SAFER, SMARTER, GREENER Wind turbine

More information

E. Agu, M. Kasperski Ruhr-University Bochum Department of Civil and Environmental Engineering Sciences

E. Agu, M. Kasperski Ruhr-University Bochum Department of Civil and Environmental Engineering Sciences EACWE 5 Florence, Italy 19 th 23 rd July 29 Flying Sphere image Museo Ideale L. Da Vinci Chasing gust fronts - wind measurements at the airport Munich, Germany E. Agu, M. Kasperski Ruhr-University Bochum

More information

The OWEZ Meteorological Mast

The OWEZ Meteorological Mast The OWEZ Meteorological Mast Analysis of mast-top displacements P.J. Eecen E. Branlard ECN-E--08-067 OWEZ_R_121_mast_top_movement Acknowledgement/Preface The Off Shore wind Farm Egmond aan Zee has a subsidy

More information

Power curves - use of spinner anemometry. Troels Friis Pedersen DTU Wind Energy Professor

Power curves - use of spinner anemometry. Troels Friis Pedersen DTU Wind Energy Professor Power curves - use of spinner anemometry Troels Friis Pedersen DTU Wind Energy Professor Spinner anemometry using the airflow over the spinner to measure wind speed, yaw misalignment and flow inclination

More information

WCA Wind Research Project Report

WCA Wind Research Project Report WCA Wind Research Project Report Steven Selvaggio Hasz Consulting Company Whitestone Community Association Presented to: Alaska Energy Authority September 25 Table of Contents I. Project Overview II. Results

More information

WIND DATA REPORT. Paxton, MA

WIND DATA REPORT. Paxton, MA WIND DATA REPORT Paxton, MA July 1, 2011 September 30, 2011 Prepared for Massachusetts Clean Energy Center 55 Summer Street, 9th Floor Boston, MA 02110 by Eric Morgan James F. Manwell Anthony F. Ellis

More information

Criteria for wind farm noise: Lmax and Lden

Criteria for wind farm noise: Lmax and Lden Criteria for wind farm noise: Lmax and Lden F. Van Den Berg University of Groningen - Science & Society Group, Nijenborgh 4, 9747AG Groningen, Netherlands fvdberg@ggd.amsterdam.nl 4043 Wind turbine noise

More information

Wind Project Siting and Permitting Blaine Loos

Wind Project Siting and Permitting Blaine Loos Wind Project Siting and Permitting Blaine Loos Energy Project Analyst Center for Wind Energy at James Madison University Wind Project Siting and Permitting The Energy in Wind Resource Assessment (Macro-siting)

More information

Wind Resource Assessment for NOME (ANVIL MOUNTAIN), ALASKA Date last modified: 5/22/06 Compiled by: Cliff Dolchok

Wind Resource Assessment for NOME (ANVIL MOUNTAIN), ALASKA Date last modified: 5/22/06 Compiled by: Cliff Dolchok 813 W. Northern Lights Blvd. Anchorage, AK 99503 Phone: 907-269-3000 Fax: 907-269-3044 www.akenergyauthority.org SITE SUMMARY Wind Resource Assessment for NOME (ANVIL MOUNTAIN), ALASKA Date last modified:

More information

Tidal influence on offshore and coastal wind resource predictions at North Sea. Barbara Jimenez 1,2, Bernhard Lange 3, and Detlev Heinemann 1.

Tidal influence on offshore and coastal wind resource predictions at North Sea. Barbara Jimenez 1,2, Bernhard Lange 3, and Detlev Heinemann 1. Tidal influence on offshore and coastal wind resource predictions at North Sea Barbara Jimenez 1,2, Bernhard Lange 3, and Detlev Heinemann 1. 1 ForWind - Center for Wind Energy Research, University of

More information

Calculation of Trail Usage from Counter Data

Calculation of Trail Usage from Counter Data 1. Introduction 1 Calculation of Trail Usage from Counter Data 1/17/17 Stephen Martin, Ph.D. Automatic counters are used on trails to measure how many people are using the trail. A fundamental question

More information

National Renewable Energy Laboratory. Wind Resource Data Summary Guam Naval Ordnance Annex Data Summary and Retrieval for November 2009

National Renewable Energy Laboratory. Wind Resource Data Summary Guam Naval Ordnance Annex Data Summary and Retrieval for November 2009 National Renewable Energy Laboratory Wind Resource Data Summary Guam Naval Ordnance Annex Data Summary and Retrieval for November 2009 Prepared for: National Renewable Energy Laboratory 1617 Cole Boulevard

More information

LONG TERM SITE WIND DATA ANNUAL REPORT. Mass Turnpike Authority Blandford, MA

LONG TERM SITE WIND DATA ANNUAL REPORT. Mass Turnpike Authority Blandford, MA LONG TERM SITE WIND DATA ANNUAL REPORT Mass Turnpike Authority Blandford, MA July 1, 2012 June 30, 2013 Prepared for Massachusetts Clean Energy Center 55 Summer Street, 9th Floor Boston, MA 02110 by Dylan

More information

Inuvik Wind Monitoring Update 2016

Inuvik Wind Monitoring Update 2016 Inuvik Wind Monitoring Update 2016 Source: MACA Prepared for By Jean Paul Pinard, P. Eng., PhD. 703 Wheeler St., Whitehorse, Yukon Y1A 2P6 Tel. (867) 336 2977; Email jpp@northwestel.net March 31, 2016

More information

Torrild - WindSIM Case study

Torrild - WindSIM Case study Torrild - WindSIM Case study Note: This study differs from the other case studies in format, while here another model; WindSIM is tested as alternative to the WAsP model. Therefore this case should be

More information

WIND DATA REPORT. Swan s Island, ME

WIND DATA REPORT. Swan s Island, ME WIND DATA REPORT Swan s Island, ME June 1, 2009 August 31, 2009 Prepared for US Department of Energy by Daniel T. Grip Utama Abdulwahid James F. Manwell Anthony F. Ellis September 17, 2009 Report template

More information

13. TIDES Tidal waters

13. TIDES Tidal waters Water levels vary in tidal and non-tidal waters: sailors should be aware that the depths shown on the charts do not always represent the actual amount of water under the boat. 13.1 Tidal waters In tidal

More information

Kodiak, Alaska Site 1 Wind Resource Report for Kodiak Electric Association

Kodiak, Alaska Site 1 Wind Resource Report for Kodiak Electric Association Kodiak, Alaska Site 1 Wind Resource Report for Kodiak Electric Association Report written by: Douglas Vaught, V3 Energy LLC, Eagle River, AK Date of report: August 23, 2006 Photo Doug Vaught General Site

More information

Oldman 2 Wind Farm Limited

Oldman 2 Wind Farm Limited Decision 22676-D01-2017 Spring 2017 Post-Construction Sound Survey at Receptors B, J and K August 1, 2017 Alberta Utilities Commission Decision 22676-D01-2017 Proceeding 22676 Application 22676-A001 August

More information

Nanortalik A preliminary analysis of the wind measurements rev 1

Nanortalik A preliminary analysis of the wind measurements rev 1 Nanortalik A preliminary analysis of the wind measurements rev 1 Introduction Note pr 14.08.2009 Tove Risberg, Kjeller Vindteknikk AS A 50 m met mast has been measuring the wind speed at Nanortalik Heliport

More information

General Accreditation Guidance. User checks and maintenance of laboratory balances

General Accreditation Guidance. User checks and maintenance of laboratory balances General Accreditation Guidance User checks and maintenance of laboratory balances January 2018 Copyright National Association of Testing Authorities, Australia 2010 All intellectual property rights in

More information

Wind Farm Power Performance Test, in the scope of the IEC

Wind Farm Power Performance Test, in the scope of the IEC Wind Farm Power Performance Test, in the scope of the IEC 61400-12.3 Helder Carvalho 1 (helder.carvalho@megajoule.pt) Miguel Gaião 2 (miguel.gaiao@edp.pt) Ricardo Guedes 1 (ricardo.guedes@megajoule.pt)

More information

WIND CONDITIONS MODELING FOR SMALL WIND TURBINES

WIND CONDITIONS MODELING FOR SMALL WIND TURBINES U.P.B. Sci. Bull., Series C, Vol. 77, Iss. 2, 2015 ISSN 2286-3540 WIND CONDITIONS MODELING FOR SMALL WIND TURBINES Viorel URSU 1, Sandor BARTHA 2 Wind energy systems are a solution which became cost effective

More information

Wind Data Verification Report Arriga 50m

Wind Data Verification Report Arriga 50m Page 1 of 11 Site Name Site Details 9531 - Arriga 5m Arriga 5m Date/Time of report generation 27/11/212 4:22 PM Site Number 9531 Mast Height 5m Mast Location 32568 E 811256 N Coordinate System UTM 55K

More information

COMPARISON OF ZEPHIR MEASUREMENTS AGAINST CUP ANEMOMETRY AND POWER CURVE ASSESSMENT

COMPARISON OF ZEPHIR MEASUREMENTS AGAINST CUP ANEMOMETRY AND POWER CURVE ASSESSMENT COMPARISON OF ZEPHIR MEASUREMENTS AGAINST CUP ANEMOMETRY AND POWER CURVE ASSESSMENT Author: Marion Cayla Issued: 8 February 2010 Natural Power, 10 place du Temple Neuf, 67000, Strasbourg, France, SIREN

More information

POWER Quantifying Correction Curve Uncertainty Through Empirical Methods

POWER Quantifying Correction Curve Uncertainty Through Empirical Methods Proceedings of the ASME 2014 Power Conference POWER2014 July 28-31, 2014, Baltimore, Maryland, USA POWER2014-32187 Quantifying Correction Curve Uncertainty Through Empirical Methods ABSTRACT Christopher

More information

Correlation analysis between UK onshore and offshore wind speeds

Correlation analysis between UK onshore and offshore wind speeds Loughborough University Institutional Repository Correlation analysis between UK onshore and offshore wind speeds This item was submitted to Loughborough University's Institutional Repository by the/an

More information

WIND DIRECTION ERROR IN THE LILLGRUND OFFSHORE WIND FARM

WIND DIRECTION ERROR IN THE LILLGRUND OFFSHORE WIND FARM WIND DIRECTION ERROR IN THE LILLGRUND OFFSHORE WIND FARM * Xi Yu*, David Infield*, Eoghan Maguireᵜ Wind Energy Systems Centre for Doctoral Training, University of Strathclyde, R3.36, Royal College Building,

More information

Yawing and performance of an offshore wind farm

Yawing and performance of an offshore wind farm Yawing and performance of an offshore wind farm Troels Friis Pedersen, Julia Gottschall, Risø DTU Jesper Runge Kristoffersen, Jan-Åke Dahlberg, Vattenfall Contact: trpe@risoe.dtu.dk, +4 2133 42 Abstract

More information

Can Lidars Measure Turbulence? Comparison Between ZephIR 300 and an IEC Compliant Anemometer Mast

Can Lidars Measure Turbulence? Comparison Between ZephIR 300 and an IEC Compliant Anemometer Mast Can Lidars Measure Turbulence? Comparison Between ZephIR 300 and an IEC Compliant Anemometer Mast W. Barker (1), M. Pitter (2), E. Burin des Roziers (3), M. Harris (4), R. Scullion (5) (1) Natural Power

More information

PUBLISHED PROJECT REPORT PPR850. Optimisation of water flow depth for SCRIM. S Brittain, P Sanders and H Viner

PUBLISHED PROJECT REPORT PPR850. Optimisation of water flow depth for SCRIM. S Brittain, P Sanders and H Viner PUBLISHED PROJECT REPORT PPR850 Optimisation of water flow depth for SCRIM S Brittain, P Sanders and H Viner Report details Report prepared for: Project/customer reference: Copyright: Highways England,

More information

Wind Assessment Basics

Wind Assessment Basics Wind Assessment Basics 120 Power curve for Northwind 100 100 80 60 40 kwh For Island Institute Fall 2013 by Mick Womersley 20 0 1 2 3 4 5 6 7 8 9 1011121314151617181920212223 Wind speed in M/S A misspent

More information

LONG TERM SITE WIND DATA QUARTERLY REPORT. Bishop and Clerks

LONG TERM SITE WIND DATA QUARTERLY REPORT. Bishop and Clerks LONG TERM SITE WIND DATA QUARTERLY REPORT Bishop and Clerks January 1, 2012 March 31, 2012 Prepared for Massachusetts Clean Energy Center 55 Summer Street, 9th Floor Boston, MA 02110 by Frederick Letson

More information

Safety Assessment of Installing Traffic Signals at High-Speed Expressway Intersections

Safety Assessment of Installing Traffic Signals at High-Speed Expressway Intersections Safety Assessment of Installing Traffic Signals at High-Speed Expressway Intersections Todd Knox Center for Transportation Research and Education Iowa State University 2901 South Loop Drive, Suite 3100

More information

FINO1 Mast Correction

FINO1 Mast Correction FINO1 Mast Correction A. Westerhellweg, T. Neunn; DEWI GmbH, Wilhelmshaven V. Riedel; DEWI North America Inc. A. Westerhellweg English Abstract Lateral speed-up effects, upwind flow retardation and downwind

More information

Flow analysis with nacellemounted

Flow analysis with nacellemounted Flow analysis with nacellemounted LiDAR E.T.G. Bot September 2016 ECN-E--16-041 Acknowledgement The work reported here is carried out in the TKI LAWINE project which is partially funded by the Dutch government

More information

Analysis and Verification of Wind Data from Ground-based LiDAR

Analysis and Verification of Wind Data from Ground-based LiDAR Analysis and Verification of Wind Data from Ground-based LiDAR Dongbum Kang*, Jiyeong Hyeon*, Kyoungboo Yang*, Jongchul Huh**, Kyungnam Ko* * Faculty of Wind Energy Engineering, Graduate School, Jeju National

More information

REAL LIFE GRAPHS M.K. HOME TUITION. Mathematics Revision Guides Level: GCSE Higher Tier

REAL LIFE GRAPHS M.K. HOME TUITION. Mathematics Revision Guides Level: GCSE Higher Tier Mathematics Revision Guides Real Life Graphs Page 1 of 19 M.K. HOME TUITION Mathematics Revision Guides Level: GCSE Higher Tier REAL LIFE GRAPHS Version: 2.1 Date: 20-10-2015 Mathematics Revision Guides

More information

To: The results of these surveys have been analysed and are summarised within this Technical Note.

To: The results of these surveys have been analysed and are summarised within this Technical Note. Technical Note Project: Histon Road / Milton Road, Cambridge Parking Surveys To: Andy Harrison Subject: Survey Report v1.6 From: Jonathan Barlow Date: 18 th February 2016 cc: Richard Jones / Dave Boddy

More information

Draft Kivalina Wind Resource Report

Draft Kivalina Wind Resource Report Draft Kivalina Wind Resource Report Kivalina aerial photo by Doug Vaught, July 2011 May 31, 2012 Douglas Vaught, P.E. dvaught@v3energy.com V3 Energy, LLC Eagle River, Alaska Draft Kivalina Wind Resource

More information

A Study of the Normal Turbulence Model in IEC

A Study of the Normal Turbulence Model in IEC WIND ENGINEERING VOLUME 36, NO. 6, 212 PP 759-766 759 A Study of the Normal Turbulence Model in 614-1 Takeshi Ishihara *,1, Atsushi Yamaguchi *,2 and Muhammad Waheed Sarwar *,3 *1 Professor, Department

More information

Valerijs Bezrukovs, Vladislavs Bezrukovs Ventspils University College Latvia. WREF2012 Denver, CO May 13-17, 2012

Valerijs Bezrukovs, Vladislavs Bezrukovs Ventspils University College Latvia. WREF2012 Denver, CO May 13-17, 2012 Valerijs Bezrukovs, Vladislavs Bezrukovs Ventspils University College Latvia WREF2012 Denver, CO May 13-17, 2012 Baltic countries 2 Currently rise of WPP development in Baltic countries. Attractive for

More information

New IEC and Site Conditions in Reality

New IEC and Site Conditions in Reality New IEC 61400-1 and Site Conditions in Reality Udo Follrichs Windtest Kaiser-Wilhelm-Koog GmbH Sommerdeich 14b, D-25709 Kaiser-Wilhelm-Koog Tel.: +49-4856-901-0, Fax: +49-4856-901-49 Axel Andreä, Kimon

More information

Anemometry. Anemometry. Wind Conventions and Characteristics. Anemometry. Wind Variability. Anemometry. Function of an anemometer:

Anemometry. Anemometry. Wind Conventions and Characteristics. Anemometry. Wind Variability. Anemometry. Function of an anemometer: Anemometry Anemometry Function of an anemometer: Measure some or all of the components of the wind vector In homogeneous terrain, vertical component is small express wind as -D horizontal vector For some

More information

Wind Regimes 1. 1 Wind Regimes

Wind Regimes 1. 1 Wind Regimes Wind Regimes 1 1 Wind Regimes The proper design of a wind turbine for a site requires an accurate characterization of the wind at the site where it will operate. This requires an understanding of the sources

More information

LONG TERM SITE WIND DATA QUARTERLY REPORT. Bishop and Clerks

LONG TERM SITE WIND DATA QUARTERLY REPORT. Bishop and Clerks LONG TERM SITE WIND DATA QUARTERLY REPORT Bishop and Clerks April 1, 2012 June 30, 2012 Prepared for Massachusetts Clean Energy Center 55 Summer Street, 9th Floor Boston, MA 02110 by Frederick Letson James

More information

WIND DATA REPORT. Quincy DPW, MA

WIND DATA REPORT. Quincy DPW, MA WIND DATA REPORT Quincy DPW, MA March 1 st 2007 to May 31 st 2007 Prepared for Massachusetts Technology Collaborative 75 North Drive Westborough, MA 01581 by James R. Browning James F. Manwell Anthony

More information

Wind Monitoring Update for Tuktoyaktuk, Winter 2009

Wind Monitoring Update for Tuktoyaktuk, Winter 2009 Wind Monitoring Update for Tuktoyaktuk, Winter 2009 Prepared for by Jean-Paul Pinard, P. Eng., Ph.D. 703 Wheeler St., Whitehorse, Yukon Y1A 2P6 Phone: (867) 393-2977 E-mail: jpp@northwestel.net Acknowledgement

More information

Wind Resource Assessment Østerild National Test Centre for Large Wind Turbines

Wind Resource Assessment Østerild National Test Centre for Large Wind Turbines Downloaded from orbit.dtu.dk on: Jan 21, 2018 Wind Resource Assessment Østerild National Test Centre for Large Wind Turbines Hansen, Brian Ohrbeck; Courtney, Michael; Mortensen, Niels Gylling Publication

More information

Atmospheric Rossby Waves in Fall 2011: Analysis of Zonal Wind Speed and 500hPa Heights in the Northern and Southern Hemispheres

Atmospheric Rossby Waves in Fall 2011: Analysis of Zonal Wind Speed and 500hPa Heights in the Northern and Southern Hemispheres Atmospheric Rossby Waves in Fall 211: Analysis of Zonal Wind Speed and 5hPa Heights in the Northern and Southern s Samuel Cook, Craig Eckstein, and Samantha Santeiu Department of Atmospheric and Geological

More information

Surf Survey Summary Report

Surf Survey Summary Report Port Otago Limited 15 Beach Street Port Chalmers Surf Survey Summary Report August 13-September 1 Leigh McKenzie Summary of Surf Locations of Interest Port Otago Ltd is undertaking monitoring of changes

More information

COMPARISON OF DIFFERENTIAL PRESSURE SENSING TECHNOLOGIES IN HOSPITAL ISOLATION ROOMS AND OTHER CRITICAL ENVIRONMENT APPLICATIONS

COMPARISON OF DIFFERENTIAL PRESSURE SENSING TECHNOLOGIES IN HOSPITAL ISOLATION ROOMS AND OTHER CRITICAL ENVIRONMENT APPLICATIONS COMPARISON OF DIFFERENTIAL PRESSURE SENSING TECHNOLOGIES IN HOSPITAL ISOLATION ROOMS AND OTHER CRITICAL ENVIRONMENT APPLICATIONS APPLICATION NOTE LC-136 Introduction Specialized spaces often times must

More information

DIRECTION DEPENDENCY OF OFFSHORE TURBULENCE INTENSITY IN THE GERMAN BIGHT

DIRECTION DEPENDENCY OF OFFSHORE TURBULENCE INTENSITY IN THE GERMAN BIGHT 10 th Wind Energy Conference DEWEK 2010 DIRECTION DEPENDENCY OF OFFSHORE TURBULENCE INTENSITY IN THE GERMAN BIGHT Annette Westerhellweg, Beatriz Canadillas, Thomas Neumann DEWI GmbH, Wilhelmshaven, Germany,

More information

Kake, Alaska Wind Resource Report

Kake, Alaska Wind Resource Report Kake, Alaska Wind Resource Report Kake met tower, photo provided by SEACC January 6, 2012 Douglas Vaught, P.E. V3 Energy, LLC Eagle River, Alaska Kake, Alaska Met Tower Wind Resource Report Page 2 Project

More information

Amplitude Modulation of Wind Turbine Noise. A Review of the Evidence

Amplitude Modulation of Wind Turbine Noise. A Review of the Evidence Amplitude Modulation of Wind Turbine Noise. A Review of the Evidence Dick Bowdler New Acoustics, 34 Old Mill Road Duntocher, Clydebank, G81 6BX, UK dick@newacoustics.co.uk 1. Introduction Many of the complaints

More information

Measurement and simulation of the flow field around a triangular lattice meteorological mast

Measurement and simulation of the flow field around a triangular lattice meteorological mast Measurement and simulation of the flow field around a triangular lattice meteorological mast Matthew Stickland 1, Thomas Scanlon 1, Sylvie Fabre 1, Andrew Oldroyd 2 and Detlef Kindler 3 1. Department of

More information

FUNCTIONAL SKILLS MATHEMATICS (level 1)

FUNCTIONAL SKILLS MATHEMATICS (level 1) FUNCTIONAL SKILLS MATHEMATICS (level 1) Detailed Marking Instructions Version: May 2011 Question Marking Scheme Illustrations of evidence No Give for each for awarding a mark 1 (a) Ans: 675 represent:

More information

HOUTEN WIND FARM WIND RESOURCE ASSESSMENT

HOUTEN WIND FARM WIND RESOURCE ASSESSMENT CIRCE CIRCE Building Campus Río Ebro University de Zaragoza Mariano Esquillor Gómez, 15 50018 Zaragoza Tel.: 976 761 863 Fax: 976 732 078 www.fcirce.es HOUTEN WIND FARM WIND RESOURCE ASSESSMENT CIRCE AIRE

More information

Wind Speed and Energy at Different Heights on the Latvian Coast of the Baltic Sea

Wind Speed and Energy at Different Heights on the Latvian Coast of the Baltic Sea J. Energy Power Sources Vol. 1, No. 2, 2014, pp. 106-113 Received: July 1, 2014, Published: August 30, 2014 Journal of Energy and Power Sources www.ethanpublishing.com Wind Speed and Energy at Different

More information

EMPOWERING OFFSHORE WINDFARMS BY RELIABLE MEASUREMENTS

EMPOWERING OFFSHORE WINDFARMS BY RELIABLE MEASUREMENTS EMPOWERING OFFSHORE WINDFARMS BY RELIABLE MEASUREMENTS Joerg Bendfeld University of Paderborn Fakultät Elektrotechnik, Mathematik und Informatik Lehrstuhl für Elektrische Energietechnik Pohlweg 55 D-33014

More information